Add to ORKGValence approximation glueball mass and decay calculations support the identification of $f_J(1710)$ as the lightest scalar glueball. An alternate glueball candidate is $f_0(1500)$. I present evidence for the identification of $f_0(1500)$ as $s\overline{s}$ quarkonium
Based on a $3\times3$ mass matrix describing the mixing of the scalar states $f_0(1370)$, $f_0(1500)...
For the first time a complete data set of the two-body decays of the f0(1370), f0(1500) and f0(1710)...
The search for the ground state scalar glueball G_0 is reviewed. Spin zero glueballs will have uniqu...
We evaluate the continuum limit of the valence (quenched) approximation to the mass of the lightest ...
I briefly review lattice QCD, the valence (quenched) approximation, and the application of both to t...
We evaluate the continuum limit of the valence approximation to the mass of scalar quarkonium and to...
We compute from lattice QCD in the valence (quenched) approximation the partial decay widths of the ...
It is commonly believed that the lowest-lying scalar glueball lies somewhere in the isosinglet scala...
The ratios of partial widths for the decay of a glueball into two pseudoscalar mesons are calculated...
A simple mixing scheme describing the $f_0(1500)$ and the $f_0(1700)$ as mixed states of a $\bar s s...
According to the QCD expectations the lightest glueball should be a scalar particle (J^{PC}=0^{++})....
The isosinglet scalar mesons $f_0(1710)$, $f_0(1500)$, $f_0(1370)$ and their mixing are studied. We ...
In our phenomenological analysis of the spectroscopy of light scalar mesons we do not find compellin...
Mass ratios of glueballs predicted by the latest Lattice QCD calculations in the quenched approximat...
The isosinglet scalar mesons $f_0(1710)$, $f_0(1500)$, $f_0(1370)$ and their mixing are studied. Two...
Based on a $3\times3$ mass matrix describing the mixing of the scalar states $f_0(1370)$, $f_0(1500)...
For the first time a complete data set of the two-body decays of the f0(1370), f0(1500) and f0(1710)...
The search for the ground state scalar glueball G_0 is reviewed. Spin zero glueballs will have uniqu...
We evaluate the continuum limit of the valence (quenched) approximation to the mass of the lightest ...
I briefly review lattice QCD, the valence (quenched) approximation, and the application of both to t...
We evaluate the continuum limit of the valence approximation to the mass of scalar quarkonium and to...
We compute from lattice QCD in the valence (quenched) approximation the partial decay widths of the ...
It is commonly believed that the lowest-lying scalar glueball lies somewhere in the isosinglet scala...
The ratios of partial widths for the decay of a glueball into two pseudoscalar mesons are calculated...
A simple mixing scheme describing the $f_0(1500)$ and the $f_0(1700)$ as mixed states of a $\bar s s...
According to the QCD expectations the lightest glueball should be a scalar particle (J^{PC}=0^{++})....
The isosinglet scalar mesons $f_0(1710)$, $f_0(1500)$, $f_0(1370)$ and their mixing are studied. We ...
In our phenomenological analysis of the spectroscopy of light scalar mesons we do not find compellin...
Mass ratios of glueballs predicted by the latest Lattice QCD calculations in the quenched approximat...
The isosinglet scalar mesons $f_0(1710)$, $f_0(1500)$, $f_0(1370)$ and their mixing are studied. Two...
Based on a $3\times3$ mass matrix describing the mixing of the scalar states $f_0(1370)$, $f_0(1500)...
For the first time a complete data set of the two-body decays of the f0(1370), f0(1500) and f0(1710)...
The search for the ground state scalar glueball G_0 is reviewed. Spin zero glueballs will have uniqu...